Early Physics at the LHC, Sheffield May 08 1 LHC News • End of June: The LHC is expected to be cooled down • End of July: First particles may be injected, and the commissioning with beams and collisions will start. • Sept/Oct: First collisions at 10 TeV. Cooldown status 13/5/08
LHC News. End of June: The LHC is expected to be cooled down End of July: First particles may be injected, and the commissioning with beams and collisions will start. Sept/Oct: First collisions at 10 TeV. Cooldown status 13/5/08. Magnet tests. Sector 4-5 Power Tests - PowerPoint PPT Presentation
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Early Physics at the LHC, Sheffield May 08 1
LHC News
• End of June: The LHC is expected to be cooled down
• End of July: First particles may be injected, and the commissioning with beams and collisions will start.
• Sept/Oct: First collisions at 10 TeV.
Cooldown status 13/5/08
Early Physics at the LHC, Sheffield May 08 2
Magnet tests
• Sector 4-5 Power Tests
• Several training quenches were observed above 5 TeV equivalent currents
• Stable conditions~10 TeVHopefully!
• The magnet training for full 14 TeV operation will then be completed over the winter shutdown 2008 - 2009
Ramp of 138 power converters to a current equivalent
to 5.3 TeV (including all high current magnets realistic LHC
optics )
Early Physics at the LHC, Sheffield May 08 3
What are minimum bias events?
• Minimum bias are inelastic collisions of two protons– Includes very rare high-pt scatters and very common low-pt scatters
• Minimum bias is an experimental definition– Defined by experimental trigger and analysis
• Relation between experiment and physics is:
inelasticndinelasticndddddsdsdmeasuredfff
fi are acceptances for different physics processes determined by the trigger Trigger bias
Early Physics at the LHC, Sheffield May 08 4
Triggering Minimum bias
Two Triggers implemented:1. Random+track triggerL1 Filled bunch triggerBunch crossing rate 13.3MHz Mean no events/crossing=0.06 94:6 empty:interaction
Use L2 pixel and SCT spacepoints to reject empty events
Use tracks in EF to reject beam-gas
75ns @ L=1031cm-2s-1 mean # of interactions/crossing ~0.06
2. L1 using Minimum bias trigger scintillators
Early Physics at the LHC, Sheffield May 08 5
MBTS
• Trigger scintillation counters mounted on end of LAr calorimeter covering same radii as ID– Cover 2<||<4
• Can be used for first data BUT!– Not rad-hard– Uses 1/8th of tilecal readout Lifetime unknown
• At L1 S/N is ‘modest’ – Now in simulation can be tuned to
measurement in the summer• Can do better at L2 with precision readout
ηη=2.0=2.0
ηη=3.8=3.8interactiointeraction pointn point
Beam-pipeBeam-pipe
++ηη
pan
nel
pan
nel
MBTMBTSS
UA5
Early Physics at the LHC, Sheffield May 08 6
MBTS trigger: Trigger bias
• MBTS_1_1 requires hits in both hemispheresThis should be similar to earlier NSD triggers
• MBTS_2 requires two paddles to be hit, can be same side• Trigger bias = efficiency of trigger for specific process
Not trigger rates!
preliminary preliminary
Will Bell
Early Physics at the LHC, Sheffield May 08 7
Inner Detector Trigger at L2
preliminary
preliminary
Use pixel and SCT spacepoints to reject empty eventsEmpty:Interaction ~ 94:6Still have large beamgas contribution
Technical details:Release 13.0.40 low pT trackingNow improved – see later
Early Physics at the LHC, Sheffield May 08 11
Minimum bias distributions
PYTHIA
Minimum bias sampleSelected by MBTS_2Corrections for:• track reconstruction• vertex reconstruction
•Multi-vertex events not looked at!
NSD sample
Distributions have pT>150MeV
6%
preliminary
preliminary
MB sample
NSD sampleCorrected for trigger bias-- change trigger bias
ATLAS has the tools to trigger on and reconstruct minimum bias events
Early Physics at the LHC, Sheffield May 08 12
Particle Composition
MB particle dominiated by low pT pions and ~10% K
• Pions– 150MeV can traverse to edge of SCT but
reduced efficiency due to inelastic collisions in ID
• Kaons– Much larger inefficiencies due to increased
inelastic collisions in ID
Efficiencies depend on relative rates of particle production in MB interactions
(Sadly CMS can do PID with analog readout)
Ian Dawson
Early Physics at the LHC, Sheffield May 08 13
0.1 < PT ≤ 0.5 (GeV)
Coming soon: Improved low pT tracking
Improved low pT turn-on
Based on two-pass tracking1. Find tracks with pT>500 MeV2. Find tracks with 100<pT<500MeV
from remaining hits, widens track finding roads
Early Physics at the LHC, Sheffield May 08 14
0.1 < PT ≤ 0.5 (GeV)
Coming Soon: Improved low pT tracking
Early Physics at the LHC, Sheffield May 08 15
Track Reconstruction efficiencies by track
insertion•Insert a track into a minimum bias event by overlapping an RDO-DIGI file of a single track event.
•Reconstruct merged event and look for inserted single track to determine efficiency.
•Uses InDetOverlay-00-00-02 (by Andrei Gaponenko)
D.Clements
Muons pT>0.5GeV
Muons pT>0.5GeV
Early Physics at the LHC, Sheffield May 08 16
PHOJET
PHOJET implemented in ATHENAImportant for systematic cross-checks
Early Physics at the LHC, Sheffield May 08 17
More work to be done
• Release 14• Multi-vertex analysis• Identification of SD, DD, ND?• Alignment study
Early Physics at the LHC, Sheffield May 08 18
Startup Conditions• Current expectations: 2 months single beam running from the end of
July– Beam stability poor
• Single beam running provides:– ‘Clean’ environment to study beam backgrounds: Beam halo and beam
gas– Alignment and commissioning of endcap systems
• When to switch-on?• Aim to trigger on beam gas and beam halo events
– Beam gas events distributed along Z following gas density– Beam halo events mainly coming from upstream tertiary collimators
(TCT)
n
Early Physics at the LHC, Sheffield May 08 19
L1 for single-beam running
• Make a trigger decision from a loose time coincidence between Beam Pickup (BPTX) and– 2 or more Minimum bias trigger scintillators (MBTS) above threshold
(MBTS overlaps EC-SCT)
OR
– 1 or more BCM above threshold
• The HV of the TGCs will be switched on when the beam is stable enough.
• The TGCs may be used to trigger on beam halo by faking a hit in the TGC1 station.– This is similar to the current cosmic setup in the barrel.
Early Physics at the LHC, Sheffield May 08 20
Track Reconstruction
• Beam halo tracks can be reconstructed by using cosmic style tracking code